A solid clathrate hydrate comprising lactate anion and a calcium cation. The clathrate hydrate serves as a sponge that can be used to store a gas such as hydrogen, methane, oxygen, or carbon dioxide. The presence of carboxylate anion (lactate) stabilizes the clathrate so that it is solid and stable at relatively mild temperatures and pressures.

Patent
   7553996
Priority
Mar 06 2007
Filed
Mar 06 2007
Issued
Jun 30 2009
Expiry
Jan 22 2028
Extension
322 days
Assg.orig
Entity
Small
6
7
EXPIRED
1. A solid clathrate hydrate comprising lactate anion and calcium cation.
18. A solid si clathrate hydrate comprising
a carboxylate anion;
a cation; and
a gas having a molecular diameter of 6 Å or less,
said clathrate hydrate being characterized in that said gas comprises at least 5% by weight of the clathrate hydrate;
and said clathrate is solid and stable ata temperature of 10° C. and a pressure of 165 psi.
2. The solid clathrate hydrate of claim 1 further comprising a gas stored in said clathrate hydrate.
3. The solid clathrate of claim 1 or claim 2 in which said clathrate is solid and stable at a temperature of 10° C. and a pressure of 14.7 psi.
4. The solid clathrate of claim 2 in which the gas is characterized by a molecular diameter of 6 Å or less.
5. The solid clathrate of claim 2 in which the gas is selected from methane, hydrogen, oxygen, and carbon dioxide.
6. The solid clathrate of claim 2 in which said gas comprises at least 5% of the clathrate by weight (gravimetric).
7. The solid clathrate of claim 1 or claim 2 further comprising a cation selected from the group consisting of sodium, potassium and magnesium.
8. The solid clathrate of claim 2 in which said gas is present at a density of at least 3 g/l in said clathrate.
9. The solid clathrate of claim 2 in which said gas is hydrogen.
10. The solid clathrate of claim 2 in which said gas is oxygen.
11. The solid clathrate of claim 2 in which said gas is methane.
12. The solid clathrate of claim 1 further comprising acetate.
13. The solid clathrate of claim 1 in which said clathrate exhibits a long broad peak above 3000 cm−1 in Raman spectrometry for the O—H stretching mode.
14. The solid clathrate of claim 1 further characterized in that said clathrate is an si clathrate structure.
15. The solid clathrate of any of claims 1, 2 or 4 wherein the unit cell volume is between 300 and 500 Å3.
16. The solid clathrate of claim 2 in which the gas is carbon dioxide.
17. The solid clathrate of claim 16 in which the clathrate further comprises sodium cation.

The general field of this invention is the storage of gases in clathrate structures.

Clathrates are solid cage-like structures in which hydrogen bonding between molecules forms a lattice of host molecules that trap and contain other molecules termed guest molecules. For example, a gas clathrate hydrate is composed primarily of water molecules that form a lattice enclosing and trapping a gas.

Clathrates typically form at low temperature and high pressure.1 Guest molecules (in addition to a gas) can stabilize the clathrate to higher temperatures and pressures.2 1 Raman Spectroscopic Investigation of CO2 Clathrate Formation, a Thesis, Patric Benziher, Ohio State University 2004.2 “Hydrogen Clusters in Clathrate Hydrates”, Mao, W. L. et al, Science, Vol. 297, pages 2247-2249 (2002).

Different structural arrangements of clathrates are distinguished by their unit cells—i.e., repeating structures of their respective lattice networks.

One clathrate structure, termed “sII”, is well studied. See, for example, “Inorganic Clathrates for Hydrogen Storage”, Struzhkin et al, Hydrogen Program Annual Review, DOE 2005 Carnegie Institute Washington. The sII unit cell is made up of 16 pentagonal dodecahedrons and 8 pentakaidecahedrons, respectively designated the small cage and large cage. Typically, large guest molecules occupy the large cage, leaving the small cage for gas storage. Struzhkin et al. cited above. The large proportion of 512 cavities in sII clathrates is thought responsible for the similarities in the Raman spectra to gas saturated water: the sII clathrate has a peak in Raman analysis at the 3100 cm−1 region. See, Mao et al., cited above.

U.S. Pat. No. 6,735,960 (hereby incorporated by reference in total) includes figures (FIGS. 5A, 5B, and 5C) depicting an sII crystal clathrate structure. The structure is characterized by cubic crystals containing sixteen 512 cavities, eight larger 51264 cavities. The tetrahedral 51264 cavities form an open tetrahedral network, with their centers arranged in a structure analogous to that of cubic ice, separated by groups of three 512 cavities. FIG. 5B of '960 shows four hydrogen molecules in one of the larger 51264 cavities and FIG. 5C of '960 shows two hydrogen molecules in one of the smaller 512 cavities. The unit cell contains 136 H2O molecules and 64 H2 molecules for a ratio of hydrogen/water=0.47. The '960 patent reports that the sII clathrate structure vanished above 115° K (at 10 kPa), but, at higher pressure (200 Mpa), the structure is stable to 280° K.

A second clathrate structure, termed “sI”, exhibits a long broad peak above 3000 cm−1 in Raman spectrometry for the O—H stretching mode.3 In the sI structure, linear tetrakaidecahedral (51262) cavities form three orthogonal axes holding a dodecahedral cavity wherever they cross (ratio 6:2 respectively per unit cell); each dodecahedral cavity sitting (in a body-centered cubic arrangement) within a cube formed by six tetrakaidecahedral (51262) cavities. These (51262) cavities join at their hexagonal faces to form columns. 3 “In Situ Observations of Methane Hydrate Formation Mechanisms in Raman Spectroscopy”, Uchida et al, Annals New York Academy of Sciences, p 593-601 (DATE?).

A third clathrate structure is termed “sH”.

The following tables present some clathrate properties.4 4 http://www.lsbu.ac.uk/water/clathrat2.html.

Characteristic properties of the clathrates
Space
Type Lattice group Unit cell Unit cell formula5
Clathrate I Cubic Pm3n a = 1.20 nm (S)2•(L)6•46H2O
Clathrate II Face- Fd3m a = 1.73 nm (S)16(L+)8•136H2O
centered
cubic
Clathrate H Hexagonal P6/mmm a = 1.23 nm (S)5(L++)•34H2O
c = 1.02 nm
5Not all cavities would normally be filled; S = small guest; L = large guest; L+ = larger guest; L++ = largest guest

Clathrate Unit Cells
Cavity 512 51262 51264 51268 435663
H2O 20 24 28 36 20
Mean cavity 3.95 4.33 4.73 5.71 4.06
radius, Å
free volume, 51 77 120 213 44
3
Clathrate 2 6
I,/unit cell
Clathrate 16 8
II,/unit cell
Clathrate 3 1 2
H,/unit cell
Guest Ar, O2, CO2, C3H8, (CH3)3CC2H5 CH4
molecules, N2, CH4 C2H6 (CH3)3CH
e.g. 1.8-2.2 1.8-2.7 2.8-3.1 3.5-4.3 1.8
approximate
radius, Å

Feil et al, The Polyhedral Clathrate Hydrates. Part 2. Structure of the Hydrate Tetra Iso-amyl Ammonium Fluoride, Journal of Chemical Physics, Vol 35 No 5 November 1961 review various gas/clathrate structures including a hydrate of tetra iso-amyl ammonium fluoride. The authors postulate that anions and cations substitute for the oxygen in the clathrate structure.

In addition to the '960 patent discussed above concerning storage of H2 in an sII clathrate, there are other reports of clathrate gas storage. Storage of H2 in an SII clathrate is disclosed in “Inorganic Clathrates for Hydrogen Storage”, Struzhkin et al, Hydrogen Program Annual Review, DOE 2005 Carnegie Institute Washington. Florusse et al. Science Vol. 306, pp. 469-471 (2004) discloses hydrogen storage in a binary SII clathrate hydrate with tetrahydrofuran (THF).

Uchida et al, report6 that methane forms an sI clathrate, although methane hydrates are generally thought to decompose at standard conditions making recovery difficult. The authors conclude, 6 “In Situ Observations of Methane Hydrate Formation Mechanisms in Raman Spectroscopy”, Uchida et al. Annals New York Academy of Sciences, p 593-601 (2004)

In a May 16-19 2006 Program Review, Rovetto et al. of the Colorado School of Mines Center for Hydrate Research report storage of H2 in sII clathrates stabilized by tetrahydrofuran, cyclohexanone, tetra-n-butylammonium bromide. They also reference a methane p-toluene sulfonic acid structure

One aspect of the invention generally features a solid clathrate hydrate comprising lactate anion and a calcium cation. In this aspect of the invention, the clathrate hydrate is, in effect, a sponge that can be used to store a gas. The presence of the carboxylate (lactate) anion stabilizes the clathrate so that it is solid and stable at relatively mild temperatures and pressures, e.g. at 10° C. and 165 psi (11.2 standard atmospheres); in fact, the clathrate is stabilized even at much lower pressures, such as 1 atmosphere (14.7 psi). Preferably the clathrate exhibits a long broad peak above 3000 cm-1 in Raman spectrometry for the O—H stretching mode. That and other factors are consistent with an sI clathrate structure and not with other known structures.

The carboxylate clathrates efficiently store gases whose molecular diameter is 5 Å or less. Hydrogen, methane and oxygen are particularly good candidates for storage by this method. The efficiency of gas storage is very good and can be 3% by weight or even higher, for example 5% or even 8% or higher.

An additional cation such has sodium, potassium or magnesium can be included to a limited extent. Acetate can also be included, along with lactate.

Another aspect of the invention generally features a solid sI clathrate hydrate comprising a carboxylate anion; a cation; and a gas having a molecular diameter of 5 Å or less. The gas comprises at least 5% by weight of the clathrate hydrate, and the clathrate is solid and stable at 10° C. and 165 psi.

Also preferably, the clathrate hydrate is a man-made structure, for example it is substantially free of components of sea water that may be found with naturally occurring clathrates such as high levels of chlorine or iodine.

The clathrates described above can be used in methods of gas storage, by providing the solid clathrate and adding the gas to the solid clathrate. The gas storage can be a renewable process, in which, after adding the gas to the solid clathrate, at least some of the gas is released (e.g., to fuel apparatus for converting the gas to mechanical or electrical energy, such as a fuel cell or an internal combustion engine). Thereafter gas is added to recharge the gas-depleted clathrate. The end user may simply exchange a container of gas depleted clathrate for a container of clathrate charged with gas.

The invention provides a relatively light structure with larger guest molecules occupying a relatively low percentage of cages so as to enhance the volume available for gas storage and the overall percentage of gas stored by weight and gas density. While not wanting to limit this invention to the following theory, we present the following as one way to visualize the gas clathrates that are stabilized with a carboxylate, particularly lactate.

When calcium and lactate molecules are included with the clathrate, they occupy oxygen positions in a hexagonal face of the tetrakaidecahedron structure. Further, one lactate molecule extends into one large cage of an sI unit structure and the other lactate molecule extends into an adjacent sI clathrate unit structure. This occupancy leaves five large cages and two small cages in each clathrate unit structure available for other guest gases.

The lactate molecule extending into the cage structure stabilizes the structure so that it is stable at higher temperatures and lower pressures, perhaps because these carboxylates offer a methyl group at the end of the molecule, which stabilizes the structure in a similar manner to methane in the formation of an sI clathrate, yet at surprisingly high temperatures and low pressures. For example, the lactate-containing clathrate remains stable under conditions that are relatively mild (e.g., below 165 psi at room temperature, e.g., 293-298° K).

Assuming the anion and cation occupy the traditional oxygen sites, an excess of hydrogen atoms is required to represent the remainder of the water molecules associated with the displaced oxygen atoms in the clathrate structure. Thus the pH of the clathrate solution would be slightly below neutral to supply these extra hydrogen atoms.

The invention thus stores significant amounts of the gas in a relatively dense structure. The five large cages have a mean radius of 4.33 Å, (a diameter of 8.66 Å).7 A cluster of six hydrogen molecules have a diameter of 6.57 Å. Therefore, the large cage can theoretically hold up to six molecules of H2 each. The two small cages can hold two molecules each. This gives a total potential of 32 moles of H2 per unit. The formula weight of a unit according to the invention is about 391 grams depending on the final components, providing a theoretical hydrogen storage potential of:
32(2)/(32*2+391)*100%=14.1%
7 http://www.lsbu.ac.uk/water/clathrat2.html.

Other gases of appropriate molecular diameter (6 Å or less; preferably 5.5 Å or less; most preferably 5 Å or less) can also be stored. Among the gases with a diameter of 6 Å or less are helium, neon, argon, krypton, nitrogen, oxygen, methane, xenon, ethane, carbon dioxide and carbon tetrafluoride.

Such clathrates can safely store hydrogen to power a vehicle using, for example, a fuel cell. Methane or other gas may be stored as fuel for an internal combustion engine. The reversibility of gas storage enables a method of providing the gas clathrate described above (i.e., charged with gas), subjecting the charged gas clathrate to discharging conditions, freeing the gas, and then adding gas to recharge the gas clathrate. This system could be used, for example, to fuel vehicles which would react the gas as it is released and then re-fuel at a supply station by exchanging spent clathrate for clathrate charged with gas, or by adding the gas.

The system could be used to store O2 at higher density than traditional gas storage methods (i.e., methods that simply pressurize O2 vapor), thus enabling smaller storage containers for medical oxygen or other applications that do not involve liquification.

Carbon dioxide storage could be used to reduce release of the gas into the atmosphere. Substitution of some sodium cation is desirable when storing carbon dioxide.

In general, lactate clathrates provide a dense storage medium for appropriately sized gases, because they are in solid form at relatively low pressures and relatively high temperatures. The clathrate can store amounts of the gas ranging from relatively low densities to very significant densities (3, 4, 5, 6, 8 g/l or more).

The details of one or more embodiments of the invention are set forth in the accompanying drawings and the description below. Other features, objects, and advantages of the invention will be apparent from the description and drawings, and from the claims.

FIGS. 1A-1C are Raman Spectra and FIG. 1D is an infrared spectra of a lactate clathrate.

FIGS. 2, 3, 4 and 5 show hydrogen uptake in a lactate clathrate.

Like reference symbols in the various drawings indicate like elements.

The following specific examples illustrate the invention.

Testing has shown that neutralized lactic acid with calcium hydroxide forms a clathrate structure. The molecular weight can be adjusted by substituting sodium for some of the calcium. Additionally, the molecular weight can be reduced by substituting acetic acid for some of the lactic acid. This disclosure describes the method used to produce these clathrates and chemical identification of the clathrates.

TABLE 1
Chemical Composition for Example 1
Chemical Grams Moles
Distilled water 65.1 3.6
85% Lactic Acid 40.8 0.39
Sodium Hydroxide 8.2 0.20
Calcium Hydroxide 5.2 0.07
Total 119.3 4.26

Table 1 shows the chemicals used in the first example. The lactic acid is added to half of the distilled water. The hydroxides are then added to the remaining distilled water The two mixtures are then combined. After approximately 80 minutes a fluffy white solid has formed.

Note that from an acid neutralization standpoint, there are two hydroxyl groups contributed by the calcium hydroxide. The total of the hydroxides is then
2*0.07+0.20=0.34  [1]
This is slightly less than the number of moles of lactic acid and so the pH is about 6. This incomplete neutralization of the acid supplies the extra hydrogen needed by the ionic clathrate structure.

There are four sources of water; the initial distilled water, the water that makes up 15% of the Lactic Acid, and the water formed by the neutralization of each of the hydroxides. This is shown in Table 2.

TABLE 2
Water Sources in Example 1
Chemical Moles Water Formed
Distilled water 3.6
85% Lactic Acid 0.39
Sodium Hydroxide 0.20
Calcium Hydroxide 0.14
Total 4.33

The hydration can be calculated by dividing the moles of water by the moles of lactic acid
4.33/0.39=11.1  [2]

Clathrates do not have a specific chemical formula. The final formula is dependent on what is trapped in the cage as a guest molecule. The final product for Example 1 has the formula:
0.20Na0.07Ca0.39La4.33H2O  [3]

Where “La” represents the lactate ion.

This formula [3] can be multiplied by 1/0.39 to give a formula based on one mole of lactic acid.
0.51Na0.18CaLa11.1H2O  [4]

The formula weight of formula [4] is 308.92.

The specific gravity (SG) of this material was found by displacement to be 1.284.

The unit cell volume based on one molecule of lactate is:
Formula Wt*(1024 cc/A3)/(6.023*1023*SG)=308.92 grams/mole*(1024 cc/Å3)/(6.023*1023 molecules/mole*1.284)=399.4 Å3  [5]

A portion of the solids generated in Example 1 were dried as described in Table 3.

TABLE 3
Drying Test
Initial Weight Final Weight Avg. Temperature Time, Min.
9.22 9.22 295° K N/A
10.54 6.65 342° K 227
27.86 13.18 375° K 394

In each case the solids achieved a constant weight at their respective temperatures. The samples were then submitted for Raman Spectroscopic analysis on a Perkin Elmer FTIR series with NIR FT Raman Accessory, LIMS 0627, SOP 008.07.

FIGS. 1A-1C are spectrum generated by Raman Spectrometry of FTIR of three samples generally prepared as above (samples 295, 342 and 375, respectively). Note that as the temperature is increased, the O—H vibron from 3100 cm−1 to 3600 cm−1 decreases. Simultaneously, the twin peaks in the neighborhood of 2942 cm−1 and 2990 cm−1 increase. Also the twin peaks in the neighborhood of 1429 cm−1 and 1456 cm−1 increase. The region of 2965 cm−1 to 2969 cm−1 is known to represent anti-symmetric stretching of the CH3 portion of a molecule. The 1465 cm−1 to 1466 cm−1 region is known to represent CH3 deformation. Therefore, as the water molecules are removed by drying, the CH3 portion of the molecule undergoes less inhibited structural changes. This is consistent with the methane clathrate sI structure. Also note that an sII clathrate would show a peak in the 3600 cm−1 to 3100 cm−1 region, which is not found.

FIG. 1D is an IR absorption spectrum generated on a different sample.

It is possible to substitute acetic acid for some of the lactic acid as shown in the following example.

TABLE 4
Composition Example 3
Chemical Grams Moles
Distilled water 104.3 5.76
85% Lactic Acid 20.2 0.19
Glacial Acetic Acid 21.6 0.36
Sodium Hydroxide 15.0 0.37
Calcium Hydroxide 10.2 0.14
Total 171.3 6.82

TABLE 5
Water Present in Composition of Example 3
Chemical Moles Water Formed
Distilled water 5.76
85% Lactic Acid 0.17
Glacial Acetic Acid 0.00
Sodium Hydroxide 0.37
Calcium Hydroxide 0.28
Total 6.58

The hydration can be calculated by dividing the water present by the total moles of carboxylate.
6.58/(0.19+0.36)=12.0  [6]

The final product has the formula:
0.37Na0.14Ca0.19La0.36Ac6.58H2O  [7]

Where La represents the lactate ion and Ac the acetate ion.

This formula [7] can be multiplied by 1/(0.19+0.36) to give a formula based on one mole of carboxylate.
0.67Na0.255Ca0.35La0.65Ac12.0H2O  [8]

The formula weight of formula [12] is 331.90.

The specific gravity of this material was found by displacement to be 1.210.

The unit cell volume based on one molecule of carboxylate is:
331.90*(1024 cc/Å3)/(6.023*1023*1.210)=455.4 Å3  [9]

In this example potassium has been substituted for sodium.

TABLE 6
Table 6: Chemical Composition Example 4
Chemical Grams Moles
Distilled water 94.4 5.2
85% Lactic Acid 52.7 0.50
Potassium Hydroxide 7.7 0.14
Calcium Hydroxide 12.1 0.16
Total 168.7 6.0

TABLE 7
Water Present in Example 4 Composition
Chemical Moles Water Formed
Distilled water 5.2
85% Lactic Acid 0.44
Potassium Hydroxide 0.21
Calcium Hydroxide 0.32
Total 6.17

The hydration can be calculated by dividing the moles of water by the moles of lactic acid
6.17/0.5=12.3  [10]

The final product has the formula:
0.21K0.16Ca0.5La6.17H2O  [11]

Where La represents the lactate ion.

This formula [11] can be multiplied by 1/0.5 to give a formula based on one mole of lactic acid.
0.42K0.32CaLa12.3H2O  [12]

The formula weight of formula [12] is 341.0.

The specific gravity of this material was found by displacement to be 1.248.

The unit cell volume based on one molecule of lactate is:
341.0*(1024 cc/Å3)/(6.023*1023*1.248)=453.7 Å3  [13]

Examples 5-9 demonstrate gas storage using the lactate clathrate.

TABLE 8
Equipment
Equipment Description
Cornelius Keg 19 L Stainless Steel, Pressure Rating 135 psig
Digital Pressure Switch SMC ISE4B-T1-65
Hydrogen Regulator Smith H1732
Petri Dish Pyrex 100 mm diameter

TABLE 9
Ingredients for carboxylate hydrate.
Moles Moles
Substance Grams Moles Moles water Lactate Calcium
Distilled Water 70.76 3.9 3.9
85% Lactic Acid 30.07 0.28 0.25 0.28
Ca(OH)2 10.4 0.14 0.281 0.14
Total 111.23 4.3 4.439 0.284 0.14

The carboxylic hydrate was made by combining 29.1 grams of distilled water with the lactic acid in one container. The remaining distilled water was combined with the calcium hydroxide in a second container. The two containers were then mixed and the formation reaction allowed to proceed for 130 minutes. This produced a solid hydrate with 15.6 moles of water for each mole of lactic acid and 0.49 moles of calcium per mole of lactic acid. The final specific gravity of the solid was 1.175.

The resulting formula is 0.488CaLa 15.6H2O with a formula weight of 391.0.

57.14 grams of the carboxylic hydrate was spread over the 100 mm Petri dish and placed in the bottom of the Cornelius Keg. The keg was pressurized to the initial pressure shown in Table 10. The absorption was allowed to proceed with pressure readings. When the pressure reached 90 to 91 psig, the Cornelius Keg was again pressurized to the original level. This recharging was repeated until the keg maintained a near steady pressure.

TABLE 10
Hydrogen Storage, Phase 1
Time, hours Pressure, psig
Charge 1
.283 95
1.33 94
23.5 93
34.5 92
39.5 92
43.75 91
58.5 91
59.5 90
71.42 89
Charge 2
71.5 96
82.5 95
85 94
94 93
106.5 92
115.5 91
127.5 90
Charge 3A
128.0 95
130.6 94
137.4 93
143.9 92
152.2 92
Charge 3B
153.1 91
159.4 91
163.5 91
165.1 90

FIG. 3 is a graph of hydrogen uptake over time from this recharging experiment for three charges designated Charge 1, Charge 2 and Charge 3A. Each charge was fitted to a least squares fit,

For Charge 1: Psig=94.625−0.0741 (Time)

For Charge 2: Psig=103.49−0.1076 (Time)

For Charge 3A: Psig=117.48−0.1776 (Time)

These three equations were then used to calculate the initial and final pressures for each Charge based on start and end times. These pressures were then used to calculate the number of moles of free hydrogen gas in the Cornelius Keg at each condition.

Hydrogen is almost an ideal gas. For these molar calculations, the moles of hydrogen were calculated using the Van der Waals equation
p=nRT/(V−nb)−a*(n/V)2

Where:

p=pressure Atmospheres

n=Number of moles

R=Universal Gas Constant 0.0820575 Atm L/(mole-K)

T=Temperature ° K=295

V=Volume=19 liters

a,b=Van der Waals constants

For hydrogen the Van der Waals constants are a=0.245 ATM-L2/Mol2 and b=0.0265 L/mol. Pressures were converted to psig by multiplying the pressure in atmospheres by 14.7 to get psig.

Table 11 lists the initial and final pressures and the calculated moles of hydrogen for each charge. The hydrogen uptake is the difference between the initial and final readings. The total for all three charges is also shown. This total is divided by the number of moles of carboxylate (lactate) used in the test. This is (57.14/111.23)*0.284=0.146

TABLE 11
Psig Moles H2
Charge 1
Initial 94.6 5.811
Final 89.3 5.53
Change 0.281
Charge 2
Initial 95.8 5.874
Final 89.8 5.554
Change 0.320
Charge 3A
Initial 94.8 5.823
Final 91.9 5.524
Change 0.156
Total Change 0.757
Moles H2/Mole La 5.2

The last entry in Table 11 shows that there were approximately 5 moles of hydrogen stored for each mole of lactate used in the test. This is consistent with the sI clathrate model and each molecule of carboxylate occupying one of the six large cells and one molecule of hydrogen occupying each of the other five large cages.

Storing 5 moles of hydrogen for one mole of lactate gives 5 moles of hydrogen to a formula weight of 391. This is 2.49% by weight=(10/(391+10)*100%.

FIG. 3 is a plot of the data from Table 11. The data for Charge 3B shown in FIG. 3, represents the continuation of the test. The dramatic change in uptake rate in Charge 3 is indicative of the second molecule moving into each cage. Continued testing is reported in phase 2 below. There is good agreement between the slope of the Charge 3B data and the Charge 1 data.

This section represents an extension of the testing reported above. FIG. 3 graphs the data for Phase 2 and is comparable to FIG. 2.

The least squares fit for this data is

For Charge 3B

Psig=105.14−0.0896(Time)

For Charge 4

Psig=113.53−0.0987(Time)

For Charge 5A

Psig=123.2−0.1151(Time)

Table 12 is the hydrogen uptake data for Phase 2 and is comparable to Table 10.

TABLE 12
Time, hours Pressure, psig
Charge 3B
143.9 92
152.2 92
153.1 91
159.4 91
163.5 91
165.1 90
178.4 89
Charge 4
178.7 96
183.4 96
187.8 95
203.8 93
208.1 93
212.4 92
217.1 92
227.4 91
232.0 91
233.4 90
241.3 90
251.9 89
Charge 5A
252.2 94
256.2 94
259.6 93
265.4 93
272.1 92
278.2 91

This section represents an extension of the testing reported above. Table 13 lists the data for Phase 3 and is comparable to Table 10 and 12.

The least squares fit for this data is

For Charge 5B Psig=116.95−0.0896(Time)

For Charge 6 Psig=136.08−0.1292(Time)

TABLE 13
Time, hours Pressure, psig
Charge 5B
285.5 91
288.5 91
297.5 91
298.5 90
304.3 90
309.5 89
315.5 89
316.6 88
Charge 6A
316.8 95
323.1 95
323.5 94
328.0 94
328.6 93
333.2 93
337.0 93
Charge 6B
338.8 92
345.9 92
350.0 92
354.0 91

TABLE 14
Charge 5B
Initial 92.2 5.683
Final 88.6 5.493
Change 0.190
Charge 6A
Initial 95.1 5.837
Final 92.3 5.688
Change 0.149
Total Change, Phase 3 0.339
Total Change, Phase 2 0.699
Total Change, Phase 1 0.736
Grand Total 1.774
Moles H2/Mole La 12.2

The last entry in Table 14 indicates that nearly twelve moles of hydrogen were stored for each mole of lactate. This is consistent with two moles of hydrogen being stored in each of five large cells and one mole of hydrogen stored in each small cell in an sI clathrate structure.

Storing 12 moles of hydrogen for one mole of carboxylate gives 12 moles of hydrogen to a formula weight of 391. This is 5.78% by weight=(24/(391+24)*100%.

FIG. 4 is a plot of the data from Table 14.

This section represents an extension of the testing reported above. Table 15 lists the data for Phase 4 and is comparable to Tables 11 and 14.

The least squares fit for this data is

TABLE 15
Time, hours Pressure, psig
Charge 6B
338.8 92
345.9 92
350.0 92
354.0 91
359.2 91
369.2 91
370.4 90
374.0 90
406.0 89
Charge 7
407.0 95
418.0 94
422.1 93
425.6 93
428.2 93
430.2 92
440.9 91
445.5 91
452.5 91
453.6 90
463.8 89
Charge 8A
464.5 96
468.6 96
473.1 95
477.6 95
484.4 94
490.8 94
494.5 93
503.5 92
Charge 8B
507.5 92
512.8 92
518.8 91
525.8 91
529.3 91
531.7 90

TABLE 16
Charge 6B
Initial 92.1 5.678
Final 88.8 5.503
Change 0.175
Charge 7
Initial 94.8 5.821
Final 89.1 5.519
Change 0.302
Charge 8A
Initial 96.2 5.895
Final 92.2 5.683
Change 0.212
Total Change, Phase 4 0.689
Total Change, Phase 3 0.339
Total Change, Phase 2 0.699
Total Change, Phase 1 0.76
Grand Total 2.463
Moles H2/Mole La 16.9

The last entry in Table 16 indicates that nearly seventeen moles of hydrogen were stored in each mole of lactate. This is consistent with three moles of hydrogen being stored in each of five large cells and one mole of hydrogen stored in each small cell in an sI clathrate structure.

Storing 17 moles of hydrogen for one mole of carboxylate gives 17 moles of hydrogen to a formula weight of 391. This is 8.00% by weight (34/(391+34)*100%.

FIG. 5 is a plot of the data from Table 16.

Testing has shown the ability of a carboxylic hydrate to absorb seventeen molecules of hydrogen for each molecule of carboxylate present. This is consistent with each carboxylate molecule occupying one of six large cages in the sI clathrate structure and three molecules of hydrogen occupying each of the other five large cages and one molecule of hydrogen in each of two small cages of the sI clathrate.

A number of embodiments of the invention have been described. Nevertheless, it will be understood that various modifications may be made without departing from the spirit and scope of the invention.

Conant, Lawrence D.

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